Te Substitution-Induced Structural Evolution and Thermoelectric Properties of Quasi-1D BiSeI

Zhiyao Zhang , Zuyong Feng , Jian Zhou

Adv. Mat. Sustain. Manuf. ›› 2026, Vol. 3 ›› Issue (1) : 10004

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Adv. Mat. Sustain. Manuf. ›› 2026, Vol. 3 ›› Issue (1) :10004 DOI: 10.70322/amsm.2026.10004
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Te Substitution-Induced Structural Evolution and Thermoelectric Properties of Quasi-1D BiSeI
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Abstract

Halide-chalcogenide compounds are promising candidates for thermoelectric applications owing to their low thermal conductivity and tunable electronic structures. Here, we systematically investigate Te-substituted BiSe1−xTexI (x = 0, 0.1, 0.3, 0.5). Structural and spectroscopic analyses confirm the successful incorporation of Te into the BiSeI-type framework, accompanied by lattice expansion, vibrational softening, and pronounced bandgap tuning. X-ray photoelectron spectroscopy verifies that Te occupies Se sites and modifies the local electronic environment, while electron microscopy reveals a morphology evolution from ribbon-like grains to plate-like and fragmented particles with increasing Te content. Thermoelectric measurements show that Te substitution simultaneously enhances electrical conductivity and suppresses thermal conductivity, arising from band-structure modulation, increased carrier concentration, mass fluctuation, and strengthened phonon scattering. Consequently, BiSe0.7Te0.3I achieves the highest ZT (~0.27 at 400 K), substantially higher than pristine BiSeI. This work demonstrates that heavy-element doping is an effective strategy for optimizing the thermoelectric performance of halide-chalcogenides.

Keywords

Layered halide-chalcogenides / Heavy-element doping / Bandgap narrowing / Thermoelectric performance

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Zhiyao Zhang, Zuyong Feng, Jian Zhou. Te Substitution-Induced Structural Evolution and Thermoelectric Properties of Quasi-1D BiSeI. Adv. Mat. Sustain. Manuf., 2026, 3(1): 10004 DOI:10.70322/amsm.2026.10004

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Author Contributions

Z.Z., Z.F. and J.Z. contributed to the study conception and design. Material preparation, data collection and analysis were performed by Z.Z. The first draft of the manuscript was written by Z.Z. Z.Z., Z.F. and J.Z. commented on previous versions of the manuscript. All authors read and approved the final manuscript.

Ethics Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Additional data can be provided upon request.

Funding

This work was funded by the Natural Science Foundation of Guangdong Province (Nos. 2022B1515020065 and 2023A1515010841, 2025A1515010050), and Guangzhou Science and Technology Project (No. 202102020126).

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

References

[1]

Wang J, Yin Y, Che C, Cui M. Research progress of thermoelectric materials—A review. Energies 2025, 18, 2122. DOI:10.3390/en18082122

[2]

Tan G, Zhao L-D, Kanatzidis MG. Rationally designing high-performance bulk thermoelectric materials. Chem. Rev. 2016, 116, 12123-12149. DOI:10.1021/acs.chemrev.6b00255

[3]

Jiang B, Yu Y, Cui J, Liu X, Xie L, Liao J, et al. High-entropy-stabilized chalcogenides with high thermoelectric performance. Science 2021, 371, 830-834. DOI:10.1126/science.abe1292

[4]

He J, Tritt TM. Advances in thermoelectric materials research: Looking back and moving forward. Science 2017, 357, eaak9997. DOI:10.1126/science.aak9997

[5]

Zhao LD, Lo SH, Zhang Y, Sun H, Tan G, Uher C, et al. Ultralow thermal conductivity and high thermoelectric figure of merit in SnSe crystals. Nature 2014, 508, 373-377. DOI:10.1038/nature13184

[6]

Gibson QD, Zhao T, Daniels LM, Walker HC, Daou R, Hébert S, et al. Low thermal conductivity in a modular inorganic material with bonding anisotropy and mismatch. Science 2021, 373, 1017-1022. DOI:10.1126/science.abh1619

[7]

Gibson QD, Manning TD, Zanella M, Zhao T, Murgatroyd PAE, Robertson CM, et al. Modular design via multiple anion chemistry of the high mobility van der waals semiconductor Bi4O4SeCl2. J. Am. Chem. Soc. 2020, 142, 847-856. DOI:10.1021/jacs.9b09411

[8]

Xu Y, Wang J, Su B, Deng J, Peng C, Wu C, et al. Tightly bound and room-temperature-stable excitons in van der waals degenerate-semiconductor Bi4O4SeCl2 with high charge-carrier density. Commun. Mater. 2023, 4, 69. DOI:10.1038/s43246-023-00392-1

[9]

Gibson QD, Newnham JA, Dyer MS, Robertson CM, Zanella M, Surta TW, et al. Expanding multiple anion superlattice chemistry: Synthesis, structure and properties of Bi4O4SeBr2 and Bi6O6Se2Cl2. J. Solid State Chem. 2022, 312, 123246. DOI:10.1016/j.jssc.2022.123246

[10]

Zhu YK, Sun Y, Dong X, Yin L, Liu M, Guo M, et al. General design of high-performance and textured layered thermoelectric materials via stacking of mechanically exfoliated crystals. Joule 2024, 8, 2412-2424. DOI:10.1016/j.joule.2024.05.006

[11]

Pan Y, Li J-F. Thermoelectric performance enhancement in n-type Bi2(TeSe)3 alloys owing to nanoscale inhomogeneity combined with a spark plasma-textured microstructure. NPG Asia Mater. 2016, 8, e275. DOI:10.1038/am.2016.67

[12]

Kim HS, Liu W, Chen G, Chu CW, Ren Z. Relationship between thermoelectric figure of merit and energy conversion efficiency. Proc. Natl. Acad. Sci. USA 2015, 112, 8205-8210. DOI:10.1073/pnas.1510231112

[13]

Ghosh S, Nozariasbmarz A, Lee H, Raman L, Sharma S, Smriti RB, et al. High-entropy-driven half-heusler alloys boost thermoelectric performance. Joule 2024, 8, 3303-3312. DOI:10.1016/j.joule.2024.08.008

[14]

Biswas K, He J, Blum ID, Wu CI, Hogan TP, Seidman DN, et al. High-performance bulk thermoelectrics with all-scale hierarchical architectures. Nature 2012, 489, 414-418. DOI:10.1038/nature11439

[15]

Klemens PG. The scattering of low-frequency lattice waves by static imperfections. Proc. Phys. Soc. Sect. A 1955, 68, 1113-1128. DOI:10.1088/0370-1298/68/12/303

[16]

Klemens PG. Thermal resistance due to point defects at high temperatures. Phys. Rev. 1960, 119, 507-509. DOI:10.1103/PhysRev.119.507

[17]

Peng J, Deskins WR, Malakkal L, El-Azab A. Thermal conductivity of α-U with point defects. J. Appl. Phys. 2021, 130, 185101. DOI:10.1063/5.0064259

[18]

Fu C, Bai S, Liu Y, Tang Y, Chen L, Zhao X, et al. Realizing high figure of merit in heavy-band p-type half-heusler thermoelectric materials. Nat. Commun. 2015, 6, 8144. DOI:10.1038/ncomms9144

[19]

Heremans JP, Jovovic V, Toberer ES, Saramat A, Kurosaki K, Charoenphakdee A, et al. Enhancement of thermoelectric efficiency in PbTe by distortion of the electronic density of states. Science 2008, 321, 554-557. DOI:10.1126/science.1159725

[20]

Liu Z, Gao W, Oshima H, Nagase K, Lee CH, Mori T. Maximizing the performance of n-type Mg3Bi2 based materials for room-temperature power generation and thermoelectric cooling. Nat. Commun. 2022, 13, 1120. DOI:10.1038/s41467-022-28798-4

[21]

Pei Y, Shi X, LaLonde A, Wang H, Chen L, Snyder GJ. Convergence of electronic bands for high performance bulk thermoelectrics. Nature 2011, 473, 66-69. DOI:10.1038/nature09996

[22]

Zhao T, Duan S, Dou W, Xu T, Wang X, Bai Y, et al. Edge-dominated epitaxy of topological insulator Bi2Se3 with ultrabroadband response. ACS Nano 2025, 19, 26055-26064. DOI:10.1021/acsnano.5c06699

[23]

Zhao C, Tan C, Lien DH, Song X, Amani M, Hettick M, et al. Evaporated tellurium thin films for p-type field-effect transistors and circuits. Nat. Nanotechnol. 2020, 15, 53-58. DOI:10.1038/s41565-019-0585-9

[24]

Wang Z, Tan C, Peng M, Yu Y, Zhong F, Wang P, et al. Giant infrared bulk photovoltaic effect in tellurene for broad-spectrum neuromodulation. Light Sci. Appl. 2024, 13, 277. DOI:10.1038/s41377-024-01640-w

[25]

Das A, Debnath K, Maria I, Das S, Dutta P, Swain D, et al. Influence of subvalent twin-rattler for high n-type thermoelectric performance in Bi13S18Br2 chalcohalide. J. Am. Chem. Soc. 2024, 146, 30518-30528. DOI:10.1021/jacs.4c11738

[26]

Ghorpade UV, Suryawanshi MP, Green MA, Wu T, Hao X, Ryan KM. Emerging chalcohalide materials for energy applications. Chem. Rev. 2023, 123, 327-378. DOI:10.1021/acs.chemrev.2c00422

[27]

Govindaraj P, Venugopal K. Intrinsic ultra-low lattice thermal conductivity in orthorhombic BiSI: An excellent thermoelectric material. J. Alloys Compd. 2022, 929, 167347. DOI:10.1016/j.jallcom.2022.167347

[28]

Ganose AM, Butler KT, Walsh A, Scanlon DO. Relativistic electronic structure and band alignment of BiSI and BiSeI: Candidate photovoltaic materials. J. Mater. Chem. A 2016, 4, 2060-2068. DOI:10.1039/C5TA09612J

[29]

Shi H, Ming W, Du M-H. Bismuth chalcohalides and oxyhalides as optoelectronic materials. Phys. Rev. B 2016, 93, 104108. DOI:10.1103/PhysRevB.93.104108

[30]

He Y, Zhou J. First-principles study on the ultralow lattice thermal conductivity of BiSeI. Phys. B 2022, 646, 414278. DOI:10.1016/j.physb.2022.414278

[31]

Xiong G, Liu T, Huang H, Wang J. Thermoelectric properties of janus BiXI (X = S and Se) monolayers: A first-principles study. J. Appl. Phys. 2024, 136, 185102. DOI:10.1063/5.0221109

[32]

Kunioku H, Higashi M, Abe R. Low-temperature synthesis of bismuth chalcohalides: Candidate photovoltaic materialswith easily, continuously controllable band gap. Sci. Rep. 2016, 6, 32664. DOI:10.1038/srep32664

[33]

Ran Z, Wang X, Li Y, Yang D, Zhao XG, Biswas K, et al. Bismuth and antimony-based oxyhalides and chalcohalides as potential optoelectronic materials. Npj Comput. Mater. 2018, 4, 14. DOI:10.1038/s41524-018-0071-1

[34]

Uher C, Yang J, Hu S, Morelli DT, Meisner GP. Transport properties of pure and doped M NiSn (M = Zr, Hf). Phys. Rev. B 1999, 59, 8615-8621. DOI:10.1103/PhysRevB.59.8615

[35]

Dedi, Lee PC, Wei PC, Chen YY. Thermoelectric Characteristics of A Single-Crystalline Topological Insulator Bi2Se3 Nanowire. Nanomaterials 2021, 11, 819-830. DOI:10.3390/nano11030819

[36]

Qiu B, Sun L, Ruan X. Lattice thermal conductivity reduction in Bi2Te3 quantum wires with smooth and rough surfaces: A molecular dynamics study. Phys. Rev. B 2011, 83, 35312. DOI:10.1103/PhysRevB.83.035312

[37]

Ruleova P, Plechacek T, Kasparova J, Vlcek M, Benes L, Lostak P, et al. Enhanced thermoelectric performance of n-type Bi2O2Se ceramics induced by Ge doping. J. Electron. Mater. 2018, 47, 1459-1466. DOI:10.1007/s11664-017-5952-4

[38]

Park KH, Lee S, Seo WS, Baek S, Shin DK, Kim IH. Thermoelectric properties of La-filled CoSb3 skutterudites. J. Korean Phys. Soc. 2014, 64, 1004-1008. DOI:10.3938/jkps.64.1004

[39]

Newnham JA, Zhao T, Gibson QD, Manning TD, Zanella M, Mariani E, et al. Band structure engineering of Bi4O4SeCl2 for thermoelectric applications. ACS Org. Inorg. Au 2022, 2, 405-414. DOI:10.1021/acsorginorgau.2c00018

[40]

Liu Y, Zhi J, Li W, Yang Q, Zhang L, Zhang Y. Oxide materials for thermoelectric conversion. Molecules 2023, 28, 5894. DOI:10.3390/molecules28155894

[41]

Inohara T, Okamoto Y, Yamakawa Y, Yamakage A, Takenaka K. Large thermoelectric power factor at low temperatures in one-dimensional telluride Ta4SiTe4. Appl. Phys. Lett. 2017, 110, 183901. DOI:10.1063/1.4982623

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